Large-mode-area microstructure optical fiber
A technology of micro-structured optical fiber and large mode field, which is applied in cladding optical fiber, multi-layer core/cladding optical fiber, etc., can solve the problems of reduced mode field area, reduced fundamental mode mode field area, and impact on use, and achieves Effects of low binding loss and low bending loss
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Embodiment 1
[0048] The cross-sectional structure of the optical fiber is as figure 1 shown. The matrix material is pure quartz, and the hole material is doped quartz material. Period Λ of the first type of hole 2 2 16 μm, hole diameter d 2 At 9.6 μm, the refractive index of the hole is 0.004 lower than that of the matrix material. The period Λ of the second type of hole 3 3 is 48 μm, the hole diameter d 3 At 14.4 μm, the refractive index of the hole is 0.004 lower than that of the host material. When the transmission wavelength is 1064 nm, the fundamental mode field area in the straight fiber can reach 3224 μm 2 , when the bending radius is 20 cm, the mode field area of the fundamental mode is 1210.8 μm 2 . The fiber can maintain low-loss transmission at bend radii as low as 12 cm. When the fiber is straight, its fundamental mode leakage loss is less than 0.002 dB / m, and its high-order mode loss is greater than 60 dB / m. The allowable bending angle range of the optical fiber c...
Embodiment 2
[0050] The cross-sectional structure of the optical fiber is as figure 2 shown. The matrix material is pure quartz, and the hole material is doped quartz material. The period Λ of the third type hole 4 4 is 8 μm, the hole diameter d 4 At 2.4 μm, the refractive index of the hole is 0.001 lower than that of the matrix material. Period Λ of the first type of hole 2 2 16 μm, hole diameter d 2 At 9.6 μm, the refractive index of the hole is 0.004 lower than that of the matrix material. The period Λ of the second type of hole 3 3 is 48 μm, the hole diameter d 3 At 19.2 μm, the refractive index of the hole is 0.004 lower than that of the host material. When the transmission wavelength is 1064 nm, the fundamental mode field area in straight fiber can reach 2520.7 μm 2 ; When the bending radius is 50 cm, the mode field area of the fundamental mode is 2778.6 μm 2 ; When the bending radius is 30 cm, the mode field area of the fundamental mode is 2204.5 μm 2 . When the fib...
Embodiment 3
[0052] The cross-sectional structure of the optical fiber is as figure 1 shown. Both the matrix material and the hole material are polymer materials. Period Λ of the first type of hole 2 2 10 μm, hole diameter d 2 At 6 μm, the refractive index of the hole is 0.006 lower than that of the matrix material. The period Λ of the second type of hole 3 3 30 μm, hole diameter d 3 At 12 μm, the refractive index of the hole is 0.006 lower than that of the matrix material. When the transmission wavelength is 633 nm, the fundamental mode field area can reach 1218.8 μm in straight fiber 2 . Its bend radius can be as low as 7.5 cm. When the fiber is straight, its fundamental mode leakage loss is less than 0.005 dB / m, and its high-order mode loss is greater than 20 dB / m. This polymer optical fiber with single-mode, large-mode field characteristics and low bending loss can be used in occasions requiring broadband and large-capacity communication in short-to-medium distance communicat...
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